Page 238 - Gas Adsorption Equilibria
P. 238

224                                                        Chapter 4

              The adsorption chamber is assumed to have been evacuated to as low a
          remnant gas pressure as  possible.  Upon  opening the  valve   the gas
          expands and  adsorption  occurs,  both  effects  causing  a decrease  of the gas
          pressure to a certain value     After equilibrium is attained, the piston in
          the storage  vessel is  moved  to reduce the volume of the vessel and  thus
          increase the gas pressure till its initial value   is realized again. The values
          of the  storage vessel’s volume and internal surface are denoted by   and
                 respectively. The  mass  balance of the  sorptive gas and  the  adsorbed
          phases is






          Here               is  the  amount of mass adsorbed per unit area on the inner
          surface of the storage vessel (SV).  This quantity normally can be assumed to
          be known  from calibration measurements.  Likewise    denotes the mass
          adsorbed per unit area on the sample material. This quantity can be calculated
          from (4.75) as








          Here we have assumed as in Eq. (4.75) that the storage vessel and adsorption
          chamber have  been  manufactured  from the  same  material having the  same
          surface properties so that the mass adsorbed per unit area on the inner surfaces
          of the vessels is the same for both vessels. According to Eq. (4.76) the surface
          adsorption               of the sample material is determined by two terms
          in parentheses (   ),  the  first of  which describes the mass of  gas  being
          transferred from the gas phase to the adsorbed phase on the surface (A) of the
          sample material during the experiment. The second term in parentheses (  )
          describes the  change in  the  mass adsorbed  on the  internal  surfaces of the
          vessels, i. e. areas       during the experiment. Numerical values of this
          term  often are  small  compared to  those  of the  first  term. Hence it  may  be
          neglected, but in principle  always  should be  considered as  a correction term
          which possibly should be  taken into  account.  It should be noted  that in the
          balance equation  (4.75) no terms  related to the microbalance  or  its  vessel
          occur. This is  due  to  the kind of “isobaric” experiment chosen,  namely the
          condition that the initial and the final gas pressure   within the system are
          the same and hence the respective terms cancel in the balance equation (4.75).
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